公开(公告)号：US20140293403A1

公开(公告)日：2014-10-02

申请号：US14350805

申请日：2012-09-03

申请人： Masanori Oto

发明人： Masanori Oto

IPC分类号： G02F1/377 ,  H01S3/109 ,  G02F1/355 ,  G02F1/35 ,  H01S3/067

CPC分类号： G02F1/3775 ,  G02F1/353 ,  G02F1/3551 ,  G02F1/3558 ,  G02F2001/3507 ,  G02F2001/3542 ,  G02F2201/02 ,  G02F2203/15 ,  H01S3/0675 ,  H01S3/06783 ,  H01S3/06791 ,  H01S3/109 ,  H01S5/146

摘要： A light source emits first incident light to a first polarization-reversed structure. The first polarization-reversed structure then converts the wavelength of the first incident light to emit a higher harmonic wave. A fiber coupler divides the higher harmonic wave output from the first polarization-reversed structure into output light emitted from the light source device and feedback light. The feedback light enters a second polarization-reversed structure. The second polarization-reversed structure then converts the wavelength of the feedback light to emit second incident light. The second incident light has the same wavelength as the first incident light. The second incident light enters a first wavelength converter.

摘要翻译： 光源将第一入射光发射到第一偏振反转结构。 第一偏振反转结构然后转换第一入射光的波长以发射高次谐波。 光纤耦合器将从第一偏振反转结构的高次谐波输出分为从光源装置发射的输出光和反馈光。 反馈光进入第二偏振反转结构。 第二偏振反转结构然后转换反馈光的波长以发射第二入射光。 第二入射光具有与第一入射光相同的波长。 第二入射光进入第一波长转换器。

公开(公告)号：US09417503B2

公开(公告)日：2016-08-16

申请号：US14350805

申请日：2012-09-03

申请人： Masanori Oto

发明人： Masanori Oto

IPC分类号： G02B6/00 ,  G02F1/35 ,  G02F2/02 ,  H01S3/00 ,  G02F1/377 ,  H01S3/109 ,  H01S3/067 ,  H01S5/14 ,  G02F1/355

CPC分类号： G02F1/3775 ,  G02F1/353 ,  G02F1/3551 ,  G02F1/3558 ,  G02F2001/3507 ,  G02F2001/3542 ,  G02F2201/02 ,  G02F2203/15 ,  H01S3/0675 ,  H01S3/06783 ,  H01S3/06791 ,  H01S3/109 ,  H01S5/146

摘要： A light source emits first incident light to a first polarization-reversed structure. The first polarization-reversed structure then converts the wavelength of the first incident light to emit a higher harmonic wave. A fiber coupler divides the higher harmonic wave output from the first polarization-reversed structure into output light emitted from the light source device and feedback light. The feedback light enters a second polarization-reversed structure. The second polarization-reversed structure then converts the wavelength of the feedback light to emit second incident light. The second incident light has the same wavelength as the first incident light. The second incident light enters a first wavelength converter.

摘要翻译： 光源将第一入射光发射到第一偏振反转结构。 第一偏振反转结构然后转换第一入射光的波长以发射高次谐波。 光纤耦合器将从第一偏振反转结构的高次谐波输出分为从光源装置发射的输出光和反馈光。 反馈光进入第二偏振反转结构。 第二偏振反转结构然后转换反馈光的波长以发射第二入射光。 第二入射光具有与第一入射光相同的波长。 第二入射光进入第一波长转换器。

公开(公告)号：US20050201682A1

公开(公告)日：2005-09-15

申请号：US10507014

申请日：2003-04-24

申请人： Hideo Hosono ,  Masahiro Hirano ,  Kenichi Kawamura ,  Masanori Oto

发明人： Hideo Hosono ,  Masahiro Hirano ,  Kenichi Kawamura ,  Masanori Oto

IPC分类号： G02B6/02 ,  G02B6/122 ,  G02B6/34

CPC分类号： G02B6/02133

摘要： A femtosecond laser radiation or a picosecond laser radiation output from light source 6 is split into a first beam reflected to an angle of 90 degrees by a beam splitter 7 and a straightly advancing second beam cut out by the beam splitter 7. The first beam is reflected at an angle of 90 degrees by a second reflecting mirror 9, reflected again at an angle of 90 degrees by a fourth reflecting mirror 11, and is collimated by a second lens 15 to be irradiated onto an optical fiber core wire 13 to be written. The second beam is reflected at an angle of 90 degrees by a first reflection mirror 8, reflected again at an angle of 90 degrees by a second reflection mirror 10, and is collimated by a first lens 14 to be irradiated onto the optical fiber core wire 13 to be written. The femtosecond laser output from the light source 6 is split into two by the beam splitter 7, which interfere with each other in the vicinity of the core of the optical fiber core wire 13 to generate a change in the refractive indices of the glass depending on the light intensity distribution of the interference fringes, such that the gratings are written in the core 1.

摘要翻译： 从光源6输出的飞秒激光辐射或皮秒激光辐射通过分束器7被分裂成以90度的角度反射成90度的第一光束，以及由分束器7切出的直线前进的第二光束。第一光束是 通过第二反射镜9以90度的角度反射，由第四反射镜11再次以90度的角度反射，并被第二透镜15准直照射到待被写入的光纤芯线13上 。 第二光束通过第一反射镜8以90度的角度反射，再次以90度的角度被第二反射镜10反射，并被第一透镜14准直照射到光纤芯线 13要写 从光源6输出的飞秒激光由光束分离器7分成两部分，它们在光纤芯线13的芯部附近彼此干涉，以产生玻璃的折射率随着 干涉条纹的光强度分布，使得光栅被写入核心1。

公开(公告)号：US06879436B2

公开(公告)日：2005-04-12

申请号：US10380833

申请日：2001-09-18

申请人： Masanori Oto ,  Yuuichi Morishita ,  Haruhito Noro

发明人： Masanori Oto ,  Yuuichi Morishita ,  Haruhito Noro

IPC分类号： G02F1/35 ,  H01S3/00 ,  G02B6/00 ,  G02B26/02

CPC分类号： G02F1/3511 ,  G02F2203/48 ,  G02F2203/52

摘要： In a light attenuator or its attenuating method, a nonlinear optical material and an aperture section are placed respectively on a same optical axis, between a receiving optical finder and a sending optical fiber. The nonlinear optical material receives and refracts an input light outputted from the receiving optical fiber. The aperture section has an aperture, receives the light having passed through the nonlinear optical material, and outputs constant output light to the sending optical fiber by only allowing only a part of the light to be outputted from the aperture.

摘要翻译： 在光衰减器或其衰减方法中，将非线性光学材料和孔径部分分别放置在接收光学取景器和发送光纤之间的同一光轴上。 非线性光学材料接收并折射从接收光纤输出的输入光。 开口部具有孔，接收已经通过非线性光学材料的光，并且通过仅允许从孔径输出一部分光，将恒定的输出光输出到发送光纤。